Optoelectric nuclear battery

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An optoelectric nuclear battery[ citation needed ] (also radiophotovoltaic device, radioluminescent nuclear battery [1] or radioisotope photovoltaic generator [2] ) is a type of nuclear battery in which nuclear energy is converted into light, which is then used to generate electrical energy. This is accomplished by letting the ionizing radiation emitted by the radioactive isotopes hit a luminescent material (scintillator or phosphor), which in turn emits photons that generate electricity upon striking a photovoltaic cell.

Contents

The technology was developed by researchers of the Kurchatov Institute in Moscow.[ citation needed ]

Description

A beta emitter such as technetium-99 or strontium-90 is suspended in a gas or liquid containing luminescent gas molecules of the excimer type, constituting a "dust plasma". This permits a nearly lossless emission of beta electrons from the emitting dust particles. The electrons then excite the gases whose excimer line is selected for the conversion of the radioactivity into a surrounding photovoltaic layer such that a theoretical lightweight, low-pressure, high-efficiency battery can be realized. (In practice, existing designs are heavy and involve high pressure.) These nuclides are relatively low-cost radioactive waste from nuclear power reactors. The diameter of the dust particles is so small (a few micrometers) that the electrons from the beta decay leave the dust particles nearly without loss. The surrounding weakly ionized plasma consists of gases or gas mixtures (such as krypton, argon, and xenon) with excimer lines such that a considerable amount of the energy of the beta electrons is converted into this light. The surrounding walls contain photovoltaic layers with wide forbidden zones, such as diamond, which convert the optical energy generated from the radiation into electrical energy.[ citation needed ]

A German patent [3] [4] provides a description of an optoelectric nuclear battery, which would consist of an excimer of argon, xenon, or krypton (or a mixture of two or three of them) in a pressure vessel with an internal mirrored surface, finely-ground radioisotope, and an intermittent ultrasonic stirrer, illuminating a photocell with a bandgap tuned for the excimer. When the beta-emitting nuclides (e.g., krypton-85 or argon-39) emit beta particles, they excite their own electrons in the narrow excimer band at a minimum of thermal losses, so that this radiation is converted in a high-bandgap photovoltaic layer (e.g., in p-n diamond) very efficiently into electricity. The electric power per weight, compared with existing radionuclide batteries, can then be increased by a factor 10 to 50 or more. If the pressure vessel is made from carbon fiber/epoxy, the power-to-weight ratio is said to be comparable to an air-breathing engine with fuel tanks. The advantage of this design is that precision electrode assemblies are not needed, and most beta particles escape the finely-divided bulk material to contribute to the battery's net power.

Disadvantages

The inherent risk of failure is likely to limit this device to space-based applications, where the finely-divided radioisotope source is only removed from a safe transport medium and placed in the high-pressure gas after the device has left Earth orbit.[ citation needed ]

As a DIY project

A simple betaphotovoltaic nuclear battery can be constructed from readily-available tritium vials (tritium-filled glass tubes coated with a radioluminescent phosphor) and solar cells. [5] [6] [7] One design featuring 14 22.5x3mm tritium vials produced 1.23 microwatts at a maximum powerpoint of 1.6 volts. [5] Another design combined the battery with a capacitor to power a pocket calculator for up to one minute at a time. [8]

See also

Related Research Articles

A radionuclide (radioactive nuclide, radioisotope or radioactive isotope) is a nuclide that has excess nuclear energy, making it unstable. This excess energy can be used in one of three ways: emitted from the nucleus as gamma radiation; transferred to one of its electrons to release it as a conversion electron; or used to create and emit a new particle (alpha particle or beta particle) from the nucleus. During those processes, the radionuclide is said to undergo radioactive decay. These emissions are considered ionizing radiation because they are energetic enough to liberate an electron from another atom. The radioactive decay can produce a stable nuclide or will sometimes produce a new unstable radionuclide which may undergo further decay. Radioactive decay is a random process at the level of single atoms: it is impossible to predict when one particular atom will decay. However, for a collection of atoms of a single nuclide the decay rate, and thus the half-life (t1/2) for that collection, can be calculated from their measured decay constants. The range of the half-lives of radioactive atoms has no known limits and spans a time range of over 55 orders of magnitude.

<span class="mw-page-title-main">Beta particle</span> Ionizing radiation

A beta particle, also called beta ray or beta radiation, is a high-energy, high-speed electron or positron emitted by the radioactive decay of an atomic nucleus during the process of beta decay. There are two forms of beta decay, β decay and β+ decay, which produce electrons and positrons respectively.

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<span class="mw-page-title-main">Radioisotope thermoelectric generator</span> Type of electric generator

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<span class="mw-page-title-main">Gas-filled tube</span> Assembly of electrodes at either end of an insulated tube filled with gas

A gas-filled tube, also commonly known as a discharge tube or formerly as a Plücker tube, is an arrangement of electrodes in a gas within an insulating, temperature-resistant envelope. Gas-filled tubes exploit phenomena related to electric discharge in gases, and operate by ionizing the gas with an applied voltage sufficient to cause electrical conduction by the underlying phenomena of the Townsend discharge. A gas-discharge lamp is an electric light using a gas-filled tube; these include fluorescent lamps, metal-halide lamps, sodium-vapor lamps, and neon lights. Specialized gas-filled tubes such as krytrons, thyratrons, and ignitrons are used as switching devices in electric devices.

<span class="mw-page-title-main">Neutron generator</span> Source of neutrons from linear particle accelerators

Neutron generators are neutron source devices which contain compact linear particle accelerators and that produce neutrons by fusing isotopes of hydrogen together. The fusion reactions take place in these devices by accelerating either deuterium, tritium, or a mixture of these two isotopes into a metal hydride target which also contains deuterium, tritium or a mixture of these isotopes. Fusion of deuterium atoms results in the formation of a helium-3 ion and a neutron with a kinetic energy of approximately 2.5 MeV. Fusion of a deuterium and a tritium atom results in the formation of a helium-4 ion and a neutron with a kinetic energy of approximately 14.1 MeV. Neutron generators have applications in medicine, security, and materials analysis.

<span class="mw-page-title-main">Tritium radioluminescence</span> Use of gaseous tritium to create visible light

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A betavoltaic device is a type of nuclear battery which generates electric current from beta particles (electrons) emitted from a radioactive source, using semiconductor junctions. A common source used is the hydrogen isotope tritium. Unlike most nuclear power sources which use nuclear radiation to generate heat which then is used to generate electricity, betavoltaic devices use a non-thermal conversion process, converting the electron-hole pairs produced by the ionization trail of beta particles traversing a semiconductor.

<span class="mw-page-title-main">Radioluminescence</span> Light produced in a material by bombardment with ionizing radiation

Radioluminescence is the phenomenon by which light is produced in a material by bombardment with ionizing radiation such as alpha particles, beta particles, or gamma rays. Radioluminescence is used as a low level light source for night illumination of instruments or signage. Radioluminescent paint is occasionally used for clock hands and instrument dials, enabling them to be read in the dark. Radioluminescence is also sometimes seen around high-power radiation sources, such as nuclear reactors and radioisotopes.

<span class="mw-page-title-main">Krypton fluoride laser</span>

A krypton fluoride laser is a particular type of excimer laser, which is sometimes called an exciplex laser. With its 248 nanometer wavelength, it is a deep ultraviolet laser which is commonly used in the production of semiconductor integrated circuits, industrial micromachining, and scientific research. The term excimer is short for 'excited dimer', while exciplex is short for 'excited complex'. An excimer laser typically contains a mixture of: a noble gas such as argon, krypton, or xenon; and a halogen gas such as fluorine or chlorine. Under suitably intense conditions of electromagnetic stimulation and pressure, the mixture emits a beam of coherent stimulated radiation as laser light in the ultraviolet range.

<span class="mw-page-title-main">Luminous paint</span> Paint that glows in the dark

Luminous paint or luminescent paint is paint that exhibits luminescence. In other words, it gives off visible light through fluorescence, phosphorescence, or radioluminescence. There are three types of luminous paints: fluorescent paint, phosphorescent paint and radioluminescent paint.

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A radioisotope piezoelectric generator (RPG) is a type of radioisotope generator that converts energy stored in radioactive materials into motion, which is used to generate electricity using the repeated deformation of a piezoelectric material. This approach creates a high-impedance source and, unlike chemical batteries, the devices will work at a very wide range of temperatures.

Krypton-85 (85Kr) is a radioisotope of krypton.

<span class="mw-page-title-main">Nike laser</span>

The Nike laser at the United States Naval Research Laboratory in Washington, DC is a 56-beam, 4–5 kJ per pulse electron beam pumped krypton fluoride excimer laser which operates in the ultraviolet at 248 nm with pulsewidths of a few nanoseconds. Nike was completed in the late 1980s and is used for investigations into inertial confinement fusion. By using a KrF laser with induced spatial incoherence (ISI) optical smoothing, the modulations in the laser focal profile are only 1% in one beam and < 0.3% with a 44-beam overlap. This feature is especially important for minimizing the seeding of Rayleigh-Taylor instabilities in the imploding fusion target capsule plasma.

<span class="mw-page-title-main">Radioactivity in the life sciences</span>

Radioactivity is generally used in life sciences for highly sensitive and direct measurements of biological phenomena, and for visualizing the location of biomolecules radiolabelled with a radioisotope.

References

  1. Hong, Liang; Tang, Xiao-Bin; Xu, Zhi-Heng; Liu, Yun-Peng; Chen, Da (2014-11-01). "Radioluminescent nuclear batteries with different phosphor layers". Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms. 338: 112–118. doi:10.1016/j.nimb.2014.08.005. ISSN   0168-583X.
  2. McKlveen, J. W.; Uselman, J. (1979). "Radioisotope-powered photovoltaic generator". Nuclear Technology. 43 (3): 366–372. doi:10.13182/NT79-A19224. ISSN   0029-5450.
  3. Jurewitsch, Boody, Fortov, Hoepfl (January 27, 2000). "Super-compact radionuclide battery useful for spacecraft contains radionuclide dust particles suspended in a gas or plasma (DE000019833648)". patentscope.wipo.int. Retrieved 2020-08-30.{{cite web}}: CS1 maint: multiple names: authors list (link)
  4. Jurewitsch, Boody, Fortov, Hoepfl (January 27, 2000). "Super-compact radionuclide battery useful for spacecraft contains radionuclide dust particles suspended in a gas or plasma (German Patent DE19833648)". freepatentsonline.com. Retrieved 21 February 2016.{{cite web}}: CS1 maint: multiple names: authors list (link)
  5. 1 2 NurdRage. "Make a Tritium Nuclear Battery or Radioisotope Photovoltaic Generator". instructables.com. Retrieved 2020-09-01.
  6. G. Heaton. "Tritium Nuclear Battery (Betaphotovoltaic)". hackaday.io. Retrieved 2020-09-01.
  7. Poole, Nick. "Nuclear Battery Assembly Guide". sparkfun.com. Retrieved 2020-09-01.
  8. G Heaton. "Nuclear Powered Calculator". hackaday.io. Retrieved 2020-09-01.